Название: Organic Electronics for Electrochromic Materials and Devices
Автор: Hong Meng
Издательство: John Wiley & Sons Limited
Жанр: Отраслевые издания
isbn: 9783527830626
isbn:
Figure 1.5 (a) The electrochromic contrast of a small molecule EC material.
Source: Jiang et al. [23]
, (b) sensitivity function of the human eye V(λ) and luminous efficacy vs wavelength.
Source: Fred Schubert [24]. © 2006, Cambridge University Press.
(c) The change of the lightness values from the neutral to the oxidized states.
Source: Li et al. [21]. © 2018, Royal Society of Chemistry.
Meanwhile, for some broad absorption or color‐to‐colorless EC materials, measurements on the relative luminance change (Δ%Y) during an EC switch are more realistic for exhibiting the overall EC contrast, which conveys more information on the perception of transmittance to the human eye. As an example, a luminance change curve during the redox process of black‐to‐transmissive EC materials is shown in Figure 1.5c. The lightness L* value (from 0 (black) to 100 (white)) of 37.5 (black state) increases to 60 (bleach state); therefore the Δ%Y is calculated as 22.5%.
Except for the aforementioned method for electrochemical contrast measurements, a photopically weighted value called photopic contrast was proposed by Javier Padilla et al. [26]. The photopic contrast also reflects an overall contrast during the whole visible region, which is more consistent with the real application condition. It can be calculated using the following equation:
where Tphotopic is the photopic transmittance, T(λ) is the spectral transmittance of the device, S(λ) is the normalized spectral emittance of a 6000 K blackbody, and P(λ) is the normalized spectral response of the eye. λmin and λmax define the considered range of wavelengths.
1.3.2 Switching Time
In the context of electrochromism, the switching time (t) can be defined as the time needed for EC materials to switch from one redox state to the other. It is generally followed by a square wave potential step method coupled with optical spectroscopy. Switching time depends on several parameters, such as the ability of the electrolyte to conduct ions as well as the ease of intercalation and deintercalation of ions across the EC active layer, the electrical resistances of electrolytes, and the transparent conducting films. Usually the liquid electrolyte has a lower resistance than the solid electrolyte; therefore the half device and the liquid electrolyte ECD will exhibit a rapid switching than solid ECD. Meanwhile, the large area ECD such as the large smart windows will show a lower switching compared with the small laboratory samples due to the larger electrical resistances of transparent conducting films. However, fast switching is not required in all applications, such as the switchable window technologies; the obvious color change process will increase the fun of user experience. Conversely, the sub‐second magnitude rapid switching is particularly desired for display applications.
Usually the switching times are evaluated at the λmax or 555 nm together with the EC contrast. Therefore there are two kinds of switching time. One is electrochemical switching time, as shown in Figure 1.6a, which is the time required for the current density to change by 90% or 95% between two constant voltages. Meanwhile the switching time of oxidization (toxidization) and reduction (treduction) process can be estimated from this curve. The other is optical switching time (Figure 1.6b), which defines the time needed for the transmittance to change by 90% or 95%. Correspondingly, the coloration switching time (tcoloration) and bleaching switching time (tbleaching) are recorded in this measurement. It is worth noting that the pulse length of potential step has influence in transmittance. A shorter potential step will achieve a smaller contrast, and longer potential will allow EC materials to reach stationary transmittance value in both coloration and bleaching state. But after a certain length, continuing increase the pulse length won't boost the contrast. Therefore the pulse length that just reached the highest contrast are applied to switching time as well as contrast tests.
Figure 1.6 The switching time of EC materials. (a) Electrochemical switching time.
Source: Li et al. [21]. © 2018, Royal Society of Chemistry
(b) Optical switching time.
Source: Hsiao et al. [27].
However, the aforementioned method of switching time is an experiential measurement, which has a difference in varied research groups, such as the different percentage of transmittance change (90% or 95%). Therefore, it is difficult to compare switching time data between different research groups. In recent years, Javier Padilla and coworkers proposed a standard method for calculating EC switching times. They fitted the contrast values as a function of pulse length to the following exponential increase function:
where ΔTmax represents the full‐switch contrast obtained for long pulse lengths and τ is the time constant. If switching time t is equal to τ, 63.2% of the maximum transmittance change is reached. At a time of 2.3τ, СКАЧАТЬ